{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:UIXIEAQ4ZRI5DLNH5T7R3JKNXU","short_pith_number":"pith:UIXIEAQ4","schema_version":"1.0","canonical_sha256":"a22e82021ccc51d1ada7ecff1da54dbd189686a13e023c58616331e0436d9384","source":{"kind":"arxiv","id":"nucl-ex/0303003","version":4},"attestation_state":"computed","paper":{"title":"Threshold Electrodisintegration of ^3He","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Cichocki, A. Hotta, A. Nogga, B. Asavapibhop, F. Casagrande, G. A. Peterson, H. Kamada, H. Witala, I. Nakagawa, J. Golak, J. Shaw, K. Burchesky, K. Wang, M.C. Berisso, P.E. Bosted, R.A. Miskimen, R.S. Hicks, R. Skibinski, S. Churchwell, S.E. Rock, T. Kobayashi, T. Suda, T. Tamae, W. Glockle, W. Turchinetz, X. Jiang","submitted_at":"2003-03-06T20:57:30Z","abstract_excerpt":"Cross sections were measured for the near-threshold electrodisintegration of ^3He at momentum transfer values of q=2.4, 4.4, and 4.7 fm^{-1}. From these and prior measurements the transverse and longitudinal response functions R_T and R_L were deduced. Comparisons are made against previously published and new non-relativistic A=3 calculations using the best available NN potentials. In general, for q<2 fm^{-1} these calculations accurately predict the threshold electrodisintegration of ^3He. Agreement at increasing q demands consideration of two-body terms, but discrepancies still appear at the"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"nucl-ex/0303003","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"nucl-ex","submitted_at":"2003-03-06T20:57:30Z","cross_cats_sorted":[],"title_canon_sha256":"f13b034b5970764b50aacc2d874dd2fd523d01d506b1741ee377f5d412dda0e9","abstract_canon_sha256":"6d520171333ea6dd6b35e6d1d405cf43cc0aec1d1fd4ed158e19487fa653f2e3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:17:51.851599Z","signature_b64":"ky8zJwyf/Br9W/JP9etPUxwKPCQc/If5OUaB8NM29gDK0pbculKf/BBOQkQXOavgPtZGwuB7nGc7StwwN2hKCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a22e82021ccc51d1ada7ecff1da54dbd189686a13e023c58616331e0436d9384","last_reissued_at":"2026-07-04T15:17:51.851132Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:17:51.851132Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Threshold Electrodisintegration of ^3He","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Cichocki, A. Hotta, A. Nogga, B. Asavapibhop, F. Casagrande, G. A. Peterson, H. Kamada, H. Witala, I. Nakagawa, J. Golak, J. Shaw, K. Burchesky, K. Wang, M.C. Berisso, P.E. Bosted, R.A. Miskimen, R.S. Hicks, R. Skibinski, S. Churchwell, S.E. Rock, T. Kobayashi, T. Suda, T. Tamae, W. Glockle, W. Turchinetz, X. Jiang","submitted_at":"2003-03-06T20:57:30Z","abstract_excerpt":"Cross sections were measured for the near-threshold electrodisintegration of ^3He at momentum transfer values of q=2.4, 4.4, and 4.7 fm^{-1}. From these and prior measurements the transverse and longitudinal response functions R_T and R_L were deduced. Comparisons are made against previously published and new non-relativistic A=3 calculations using the best available NN potentials. In general, for q<2 fm^{-1} these calculations accurately predict the threshold electrodisintegration of ^3He. Agreement at increasing q demands consideration of two-body terms, but discrepancies still appear at the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0303003","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/nucl-ex/0303003/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"nucl-ex/0303003","created_at":"2026-07-04T15:17:51.851195+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-ex/0303003v4","created_at":"2026-07-04T15:17:51.851195+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-ex/0303003","created_at":"2026-07-04T15:17:51.851195+00:00"},{"alias_kind":"pith_short_12","alias_value":"UIXIEAQ4ZRI5","created_at":"2026-07-04T15:17:51.851195+00:00"},{"alias_kind":"pith_short_16","alias_value":"UIXIEAQ4ZRI5DLNH","created_at":"2026-07-04T15:17:51.851195+00:00"},{"alias_kind":"pith_short_8","alias_value":"UIXIEAQ4","created_at":"2026-07-04T15:17:51.851195+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UIXIEAQ4ZRI5DLNH5T7R3JKNXU","json":"https://pith.science/pith/UIXIEAQ4ZRI5DLNH5T7R3JKNXU.json","graph_json":"https://pith.science/api/pith-number/UIXIEAQ4ZRI5DLNH5T7R3JKNXU/graph.json","events_json":"https://pith.science/api/pith-number/UIXIEAQ4ZRI5DLNH5T7R3JKNXU/events.json","paper":"https://pith.science/paper/UIXIEAQ4"},"agent_actions":{"view_html":"https://pith.science/pith/UIXIEAQ4ZRI5DLNH5T7R3JKNXU","download_json":"https://pith.science/pith/UIXIEAQ4ZRI5DLNH5T7R3JKNXU.json","view_paper":"https://pith.science/paper/UIXIEAQ4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-ex/0303003&json=true","fetch_graph":"https://pith.science/api/pith-number/UIXIEAQ4ZRI5DLNH5T7R3JKNXU/graph.json","fetch_events":"https://pith.science/api/pith-number/UIXIEAQ4ZRI5DLNH5T7R3JKNXU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UIXIEAQ4ZRI5DLNH5T7R3JKNXU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UIXIEAQ4ZRI5DLNH5T7R3JKNXU/action/storage_attestation","attest_author":"https://pith.science/pith/UIXIEAQ4ZRI5DLNH5T7R3JKNXU/action/author_attestation","sign_citation":"https://pith.science/pith/UIXIEAQ4ZRI5DLNH5T7R3JKNXU/action/citation_signature","submit_replication":"https://pith.science/pith/UIXIEAQ4ZRI5DLNH5T7R3JKNXU/action/replication_record"}},"created_at":"2026-07-04T15:17:51.851195+00:00","updated_at":"2026-07-04T15:17:51.851195+00:00"}